Wavelength converting material for a light emitting device

ABSTRACT

Embodiments of the invention include a luminescent structure including an InxZnyP core, wherein 0&lt;y/x&lt;10, and wherein the core comprises an alloy including both In and Zn, and a shell disposed on a surface of the core, wherein a difference between a lattice constant of the shell and a lattice constant of the core relative to the lattice constant of the shell is less than 1%.

CROSS-REFERENCE TO RELATED APPLICATIONS

The present application claims priority to U.S. Provisional PatentApplication No. 62/247,086, filed Oct. 27, 2015. U.S. Provisional PatentApplication No. 62/247,086 is incorporated herein.

BACKGROUND

Semiconductor light-emitting devices including light emitting diodes(LEDs), resonant cavity light emitting diodes (RCLEDs), vertical cavitylaser diodes (VCSELs), and edge emitting lasers are among the mostefficient light sources currently available. Materials systems currentlyof interest in the manufacture of high-brightness light emitting devicescapable of operation across the visible spectrum include Group III-Vsemiconductors, particularly binary, ternary, and quaternary alloys ofgallium, aluminum, indium, and nitrogen, also referred to as III-nitridematerials. Typically, III-nitride light emitting devices are fabricatedby epitaxially growing a stack of semiconductor layers of differentcompositions and dopant concentrations on a sapphire, silicon carbide,III-nitride, or other suitable substrate by metal-organic chemical vapordeposition (MOCVD), molecular beam epitaxy (MBE), or other epitaxialtechniques. The stack often includes one or more n-type layers dopedwith, for example, Si, formed over the substrate, one or more lightemitting layers in an active region formed over the n-type layer orlayers, and one or more p-type layers doped with, for example, Mg,formed over the active region. Electrical contacts are formed on the n-and p-type regions.

A light emitting device such as an LED is often combined with awavelength converting material. Colloidal semiconductor nanocrystals(NCs), also called quantum dots (QDs), have attracted considerableinterest in several fields (renewable energy, optoelectronic andbiomedical devices) due to their unique optical and electricalproperties. In particular, QDs are seen as suitable candidates toreplace current phosphors in LEDs, especially red phosphors, for generallighting as they may enhance the overall LED efficiency, due to theirnarrow-band emission, and may produce high quality white light.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates X-ray diffraction (XRD) patterns of zinc blendeIn_(x)Zn_(y)P NCs, with different Zn²⁺ concentrations.

FIG. 2 illustrates the Zn/In ratio measured via ICP-AES elementalanalysis and X-ray photoelectron spectroscopy (XPS) as a function of theamount of Zn²⁺ added in the reaction.

FIG. 3 illustrates lattice constant of In_(x)Zn_(y)P nanocrystals as afunction of the Zn²⁺ concentration.

FIG. 4 is a cross sectional view of an LED.

FIG. 5 is a cross sectional view of a device with a wavelengthconverting structure in direct contact with an LED.

FIG. 6 is a cross sectional view of a device with a wavelengthconverting structure in close proximity to an LED.

FIG. 7 is a cross sectional view of a device with a wavelengthconverting structure spaced apart from an LED.

FIGS. 8A, 8B, and 8C illustrates core-shell, giant core-shell, andasymmetric core-shell quantum dots, respectively.

FIG. 9A illustrates normalized absorption and normalized PL spectra ofIn_(x)Zn_(y)P QDs with different Zn²⁺ concentration. FIG. 9B is a plotof the λ,max (nm) for the absorption and PL emission wavelengths asfunction of the Zn/In molar ratio obtained by ICP(OES) analysis. FIG. 9Cis a plot of the PL QY (%) of In_(x)Zn_(y)P QDs as function of the Zn/Inmolar ratio obtained by ICP(OES) analysis.

FIG. 10 is a plot of absorption (left) and PL emission (right) of anIn_(x)Zn_(y)P core with Zn/In:2.8 and anIn_(x)Zn_(y)P/ZnSe_(0.51)S_(0.49) core-shell.

FIG. 11A illustrates absorption (solid line) and emission (dashed line)spectra of In_(x)Zn_(y)P/In—Ga—P/GaP/ZnSe_(z)S_(1-z) core/shell QDs atdifferent stages during the growth of a ZnSe_(z)S_(1-z) shell. FIG. 11Billustrates XRD patterns obtained from drop-cast solutions ofIn_(x)Zn_(y)P (Zn/In=1.5) QDs, In_(x)Zn_(y)P/In—Ga—P/GaP QDs, andIn_(x)Zn_(y)P/GaP/ZnSe_(z)S_(1-z) QDs. The corresponding bulkreflections of zinc blende InP, GaP, ZnSe, ZnS, are reported in thelower panels. FIG. 11C illustrates photoluminescence quantum yield forfour suspensions of QDs kept under constant UV irradiation (UV lamp (1W/cm²)), as a function of the irradiation time. Four samples weremeasured: two batches of purifiedIn_(x)Zn_(y)P/In—Ga—P/GaP/ZnSe_(x)S_(1-x) QDs,In_(x)Zn_(y)P/ZnSe_(x)S_(1-x) QDs, and In_(x)Zn_(y)P/In—Ga—P/GaP QDs.

DETAILED DESCRIPTION

The main requirements for QDs to be employed in commercial applicationsare a high photoluminescence (PL) quantum efficiency (QE), and a highstability. Among investigated materials, cadmium-based QDs, such as, forexample CdSe, represent the current state-of-the-art, and have been wellstudied for such applications. However, Cd based QDs are undesirable dueto their high toxicity. InP based QDs are recognized a promising Cd-freematerial, since they can offer a comparable emission range to that ofCd-based QDs. However, their full potential has not yet beendemonstrated as their quality (QE and stability) lags behind that of Cdbased QDs. One strategy for achieving higher PL efficiency is toepitaxially grow a shell of a wider band gap material around the QDcore, resulting in core/shell particles. In this manner, the PLefficiency and stability against photo-oxidation can be significantlyimproved. Note that the shell material must be carefully chosen so thatits properties (such as band-gap) are compatible with the intendedapplication.

One of the main problems associated with epitaxial growth of a shelllayer onto a QD core is the lattice mismatch between the core and shellmaterials, which can lead to the formation of defects at the interface.These defects can act as trap states for photogenerated charge carriers,leading to non-radiative decay and hence reduction of the PL QE. Most ofthe approaches developed to reduce or eliminate defect formation duringthe shell growth have dealt with optimizing the shell structure.

One approach is the use of multiple shells around the emissive core,CdSe/CdS/ZnS being a typical example. The outer shell is often a highband-gap material to confine the exciton, while the inner shell isdesigned to address the lattice mismatch between the core and the outershell. Another approach involves gradient alloying of the inner shelland the outer shell during the shell growth, to reduce the strain due tolattice mismatch between the inner and outer shell.

For example, in the case of CdSe/CdS or CdSe/ZnS, a gradient shell maybe formed by simultaneous addition of Se and S precursors in the case ofCdSe/CdS, or Zn and Cd precursors in the case of CdSe/ZnS. A similarapproach for the synthesis of Cd_(x)Zn_(1-x)S graded shells on CdSenanoparticles is based on interface alloying between CdS and ZnS shellsby performing the reaction at elevated temperatures (300° C.). Anintermediate layer, such as ZnSe, may serve as a “lattice adapter” (orbuffer layer) to ensure a low lattice strain. Examples of QDs with anintermediate layer include CdSe/ZnSe/ZnS and InP/GaP/ZnS.

However, these strategies increased the complexity of fabrication ofcore/shell QDs. Also, although they sometimes reduced the latticemismatch in the layered structure and hence resulted in fewerinterfacial defects, this approach aimed to reduce strain in the shellstructure. The lattice mismatch between the emissive core and the firstshell is therefore not eliminated in this approach, hence it is likelythat some interfacial defects remain near the core, where they may bemost harmful to the performance of the QDs. In addition, the formationof low lattice mismatch core-shell systems based on InP QDs has beenless successful than for Cd-based systems, which is likely a significantreason why the QE and stability of InP-based QDs has historically beenlower than for Cd-based QDs.

In embodiments of the invention, the core of a core-shell QD has acrystal lattice constant that matches or nearly matches the lattice of ashell structure, thereby reducing the problem of lattice mismatchbetween the core and the shell, potentially reducing or eliminatingdefects in the core/shell QDs, while retaining the confinement of theexcitons. In some embodiments, the lattice constant of a QD is alteredby replacing an atom in the QD with a smaller atom. In some embodiments,the replaced atom is a cation that is replaced with a cation having asmaller ionic radius. In some embodiments, the lattice constant ofInP-based QDs is altered by replacing some In³⁺ atoms inside thenanocrystals with a cation having a smaller ionic radius, such as, forexample, Zn²⁺. The second cation is introduced during the synthesis ofInP QDs. The Zn²⁺ cation incorporates into the crystal of the QDs at theIn³⁺ site in some embodiments, or in any other suitable location thatforms an alloy including both In³⁺ and Zn²⁺.

In some embodiments, the lattice constant of the InP-based alloyed QDsmay be selected to match a wide range of shell materials including, forexample, ZnSe, GaP, and ZnS. This allows the formation of fully latticematched core-shell and core-shell-shell QDs. This approach can be usedto synthesize fully lattice matched or nearly lattice matched cadmiumfree In_(x)Zn_(y)P/GaP/ZnSe_(z)S_(1-z) QDs, where x/y=0-10 and z=0-1. Insome embodiments, the core-shell QDs are entirely zinc blende crystalstructures (i.e., both the core and shell are zinc blende materials),with the lattice constant of GaP. Alternatively, in some embodiments,the lattice constant of an InP-based core may be matched or nearlymatched to that of a ZnSe_(z)S_(1-z) shell, without an intermediate GaPshell. This provides an alternative to including an intermediate GaPshell as buffer layer to accommodate the lattice mismatch between coreand outer shell. Such lattice tuned In_(x)Zn_(y)P/ZnSe_(z)S_(1-z) QDsmay exhibit PL QYs as high as In_(x)Zn_(y)P/GaP/ZnSe_(z)S_(1-z) QDs.

In some embodiments, by gradually increasing the concentration of Zn²⁺in In_(x)Zn_(y)P QDs, the crystal lattice may shrink, while beneficiallypreserving the zinc-blende crystal structure of pure InP. Zn²⁺ isincorporated into the NCs during the synthesis as a substitutionaldopant onto In³⁺ sites. The ionic radius of Zn²⁺ is 0.074 nm and theionic radius of In³⁺ is 0.081 nm, therefore the cation replacement ofIn³⁺ by Zn²⁺ leads to the lattice shrinking. Even when Zn²⁺ is used in ahigh excess in the synthesis, no side formation of secondary phases wasobserved except for the desired In_(x)Zn_(y)P phase.

FIG. 1 demonstrates that as the Zn²⁺ concentration increases, thecrystal lattice shrinks, but the structure remains zinc-blende. FIG. 1illustrates X-ray diffraction (XRD) patterns of zinc blendeIn_(x)Zn_(y)P NCs, with different Zn²⁺ concentrations. The XRD patternof bulk zinc blende InP is shown in the lower panel, and the XRDpatterns of tetragonal Zn₂P and monoclinic Zn₃P₂ are shown in the upperpanel. The Zn/In ratios shown were determined by inductively coupledplasma atomic emission spectroscopy (ICP-AES) analysis. The samplesprepared with addition of Zn precursor exhibit similar XRD reflectionsbut with a systematic shift towards higher diffraction angles as theconcentration of Zn is increased. This demonstrates that all sampleshave a zinc-blende crystal structure and that the addition of Znproduced a systematic contraction of the final crystal lattice ratherthan producing other side products, such as Zn_(x)P_(y) NCs (i.e.tetragonal or monoclinic Zn₂P, or monoclinic or cubic Zn₃P₂) that wouldexhibit clear distinguishable XRD peaks. The data illustrated in FIG. 1excludes a scenario whereby Zn only goes on the surface of the NC, suchas a dopant species, since such a scenario would not lead to a shift inthe XRD patterns.

To confirm that Zn substitutes for In, simulated XRD patterns werecompared to experimental XRD patterns. In the case of substitutionalzinc, Zn²⁺ cations were progressively introduced in the composition ofthe QD while preserving charge neutrality. To preserve chargeneutrality, In³⁺ cations were substituted by Zn²⁺ cations and one P³⁻anion was removed from the structure. In the case of interstitial zinc,two Zn²⁺ were introduced on In³⁺ sites while a third Zn²⁺ cation wasplaced in an interstitial position. Simulated XRD patterns of the Zn onsubstitutional sites show a shift at higher 2 theta that closelyresemble the experimental XRD patterns while the simulated XRD patternsof the Zn on interstitial sites deviate significantly from theexperimental results. Therefore, the results in FIG. 1 suggest that Znis incorporated substitutionally on In sites. The contraction of thelattice upon incorporation of Zn, may be explained by the smaller atomicnumber of Zn compared to In.

Regarding the actual charge of In_(x)Zn_(y)P NCs, as described above,indium cations are replaced with zinc cations, having stable oxidationstates of 3+ and 2+, respectively. In order to study if thissubstitution had any influence in the final charge of the In_(x)Zn_(y)PNCs, the ζ-potential of the NCs obtained using a Zn/In ratio of 0, 1,and 2 was measured. Within the experimental error, the measured chargewas zero for all samples. Accordingly, any charge introduced by thesubstitutional Zn²⁺ is somehow compensated. Four charge compensatingscenarios are contemplated: (i) p-doping could occur to compensate forthe net negative charge introduced by Zn²⁺ on and In³⁺ site. However,this would most likely lead to efficient Auger quenching and absorptionbleach, of which no indications are found in the UV-VIS absorption andemission measurements. (ii) Zn²⁺ could occupy both interstitial andsubstitutional positions in the NC, in this case for three Zn²⁺incorporated into the NCs only two In³⁺ sites would be occupied,preserving neutrality. The comparison between experimental and simulatedXRD patterns presented above shows that this is likely not the case.(iii) The InP QDs are passivated by negatively charged x-type palmitateligands. If the QDs become negatively charged due to Zn²⁺ on In³⁺ sites,it seems likely that this could induce the desorption of such ligandswhich would lead to charge balance. There is no evidence for or againstthis scenario. (iv) Phosphorus vacancies may form to balance the charge(one for every three In³⁺ replaced by three Zn²⁺).

There are at least two possible mechanisms for the formation of thealloy including In and Zn: (i) after the nucleation and growth of InPNCs, In³⁺ is replaced by Zn²⁺ via a cation exchange reaction; or (ii)In³⁺ and Zn²⁺ react simultaneously with P³⁻ directly forming alloyedIn_(x)Zn_(y)P NCs. A kinetic study of the synthesis was carried out bymonitoring the Zn/In ratio at different stages of the reaction viaICP(AES) (between 30 s and 2 h) for In_(x)Zn_(y)P where initialconcentrations of Zn/In=1.5 and Zn/In=4 were used. The observed Zn/Inratio was roughly constant during the whole reaction, showing a slightvariation from 1.45 to 1.80 in the case of Zn/In=⅕, and from 3.56 to3.73 in the case of Zn/In=4. This suggests that Zn²⁺ ions areincorporated into the NC from the very early stages of the reaction,leading to the formation of In_(x)Zn_(y)P alloyed NCs. Had the Zn²⁺instead exchanged the In³⁺ in preformed InP NCs, a significant increasein Zn²⁺ content at a certain stage during the reaction would have beenobserved, i.e. scenario (ii). In addition, the spectral position of thefirst absorption peak, which is intrinsically correlated to the size ofthe QDs, kept changing during the entire reaction time, showing that theNCs continued to grow.

FIG. 2 demonstrates that an InZnP alloy is formed, rather than simplyInP particles doped with Zn. FIG. 2 plots the Zn/In ratio measured viaICP-AES elemental analysis and X-ray photoelectron spectroscopy (XPS) asa function of the amount of Zn²⁺ added in the reaction. To ensure thatall the side products of the reaction were removed and that the speciesdetected were only in the QDs, the particles were washed three timeswith ethanol. As an additional washing step the organic ligands werestripped and replaced with an inorganic ligand(S²⁻). Therefore the ratiomeasured refers only to that present in the QDs. Up to Zn/In=2 thepoints follow a linear trend, whereas in the range Zn/In=2-10 a sublinear trend can be observed. However, even in the case of Zn/In=10, aratio of Zn/In=7.4 is measured in the QDs. This indicates that theparticles are not merely InP doped with Zn, but rather that a true alloyis formed. Accordingly, the composition of the particles, and thereforethe lattice spacing, may be strictly controlled. In some embodiments,during synthesis, up to a Zn/In ratio of 2 there is a one-to-onecorrespondence between the determined ratio and the precursor ratio ofIn/Zn provided during synthesis. This indicates that the Zn precursorsare quantitatively incorporated into the NCs. Increasing the amount ofZn/In precursor ratio above 2 results in experimental Zn/In ratiosslightly below the added ratio. In some experiments, the curve reachedsaturation at Zn/In ratio of ˜4, as a plateau could be observed.Accordingly, even when using high Zn/In ratio (Zn/In:10 or 20), no morethan ˜Zn/In:4 is incorporated into the NCs in some embodiments. In someembodiments, the Zn/In ratio is therefore in the range 0-5.

The technique described above permits tuning of the lattice constantbetween 5.927 nm, in the case of pure InP, to 5.542 nm in the case ofInZn₅P_(z), as illustrated in FIG. 3. FIG. 3 is plot of lattice constantof In_(x)Zn_(y)P NCs as a function of the Zn²⁺ concentration. The dashedlines indicate the lattice constant for bulk InP, ZnSe, GaP, and ZnS.The lattice constants of In_(x)Zn_(y)P were calculated using aNelson-Riley plot. It is clear from FIG. 3 that by addition of a secondcation, the core's lattice constant may be selected such that it matchesthe lattice constant of a given shell structure. Thus, In_(x)Zn_(y)Pcores can be fabricated with lattice spacing comparable to the latticespacing of shell materials such as ZnSe, GaP and ZnS. Consequently, itmay be possible to design core/shell QDs without a lattice mismatchbetween the lattices of the core and shell, or with reduced latticemismatch as compared to the prior art. This allows epitaxial growth ofthe shells potentially without the formation of interfacial defects,which may improve PL QE and PL stability. The lattice constant of thecore may be at least 5.4 Å in some embodiments, at least 5.405 Å in someembodiments, no more than 6 Å in some embodiments, no more than 5.927 Åin some embodiments, at least 5.542 Å in some embodiments, and no morethan 5.833 Å in some embodiments.

The addition of Zn may improve the PL QY, up to 20% in some embodiments.PL emission spectra show that the addition of zinc precursor has a clearinfluence on the removal of trap states of the resulting NCs. The PLemission spectrum of the pure InP QDs shows a broad secondary peak atlower energies, a peak usually associated with defect trap states. Uponthe introduction of zinc this peak is suppressed. At the same time PL QYof the alloyed QDs increases from about 0-1% in pure InP up to 20% infor Zn/In=1.5. Also, the PL decay becomes longer as the amount of zincincreases, showing that the addition of Zn decreases the rate ofnon-radiative recombination. That the addition of zinc leads to anenhancement of the PL QY might suggest that the Zn²⁺ ions, in additionto being incorporated inside the QD lattice, can also passivate thesurface of the NCs as it is known that usually the trap states in QDsare mainly located on the surface. In some embodiments, the PL QY ishighest when the lattices of core and shell are matched to each other. Amaximum PL QY of 64% was observed for In_(x)Zn_(y)P/ZnSe_(z)S_(1-z) withy/x=2 and z=0.8.

Several groups have used Zn²⁺ in the synthesis of InP quantum dots, forexample to attempt to improve the PL efficiency of the core, or toassist the shell growth. However, there is no evidence in this earlierwork that Zn²⁺ was included in the crystal lattice of the InP QDs,rather than simply present as a dopant. In addition, the earlier workdid not teach using Zn²⁺ as a tool to tune the lattice constant of theresulting NCs.

Increasing the concentration of Zn²⁺ in InP QDs may shift the PLemission to lower wavelengths. In some embodiments, the lattice-matchingcores synthesized with the above-described method may emit in thegreen-yellow region of the spectra. In some embodiments, the synthesismethod described above may be adapted to grow bigger In_(x)Zn_(y)P QDsthat can emit at higher wavelengths, for example by subsequent additionof In+Zn precursors.

In some embodiments, the InZnP core-shell materials described herein areused with an intermediate GaP layer between the In_(x)Zn_(y)P core andthe ZnSe_(z)S_(1-z) shell, hence formingIn_(x)Zn_(y)P/GaP/ZnSe_(z)S_(1-z) QDs orIn_(x)Zn_(y)P/InGaP/GaP/ZnSe_(z)S_(1-z) QDs.

One or more intermediate Ga-containing layers may be formed by adding aGa³⁺ precursor such as Ga(OA)₃ to the reaction mixture of as synthesizedIn_(x)Zn_(y)P QDs. When a small amount of Ga precursor (less than 0.12mmol) is added to zinc-containing indium phosphide QDs, in someembodiments a cation exchange reaction occurs, whereby zinc ions aregradually replaced by gallium ions starting from the surface, and, thus,forming In_(x)Zn_(y)P/In—Ga—P core/graded-shell heterostructures. As theIn—Ga—P shell forms at the expenses of the starting In_(x)Zn_(y)P NCs, ablue-shift of the exciton absorption peak (i.e. GaP has a wider bandgapin respect to InP) takes place. The In—Ga—P graded shell may passivatethe surface of the starting QDs, and/or may allow for an unstrainedmatching between the core and shell materials (the lattice mismatchbetween InP and GaP is 6.9%), thus reducing the defect density at theinterface, and, consequently, increasing the PL QY. When a large amountof Ga precursor is added (more than 0.09-0.12 mmol), the cation exchangebetween Zn²⁺ and Ga³⁺ ions goes to completion and extra gallium depositson the surface of the QDs, causing an increase in the QDs size, andtherefore a red-shift and a decrease in the PL QY.

In some embodiments, the addition of a Ga precursor may increaseparticle size, for example from 2.8±0.3 nm in case of In_(x)Zn_(y)P(Zn/In=1.5) cores to 3.5±0.3 nm for In_(x)Zn_(y)P/In—Ga—P QDs (after theaddition of 0.15 mmol of Ga(OA)₃). When little or no zinc is present inthe starting NCs, the Ga directly deposits on the surface of the QDs,generating defects at the interface and potentially impeding anyimprovement of the PL QY. In some embodiments, a Ga-containingintermediate layer is used with In_(x)Zn_(y)P cores where Zn/In≥0.5.

The inventors observed an increase in PL QY upon addition of Ga, whichis strongly dependent on the Zn concentration in starting In_(x)Zn_(y)Pnanocrystals. The best PL QY (40%) was achieved when synthesizingstarting indium phosphide QDs using a Zn/In ratio of 1.5 and adding,afterward, 0.09 mmol of Ga(OA)₃. To further enhance the PL emission ofsuch QDs a thicker GaP shell was grown. In order to overgrow a GaP shellsubsequent amounts of gallium (Ga(OA)₃) and phosphorus (P(TMS)₃)precursors were injected into the crude reaction mixture containing theas synthesized In_(x)Zn_(y)P/In—Ga—P QDs. A maximum PL QY of 55% wasreached after one addition of Ga and P precursors while further growthof the GaP shell resulted in a broadening of the PL spectra and in adecrease of the PL QY. As the GaP shell becomes thicker, the latticemismatch between the core and the shell becomes more important leadingto an increase of the lattice strain at the interface and possibly to ahigher defect density, hence causing a reduction of the PL QY.

To improve the PL emission and the photo-stability, a further shell of awider band gap material was overgrown onto the In_(x)Zn_(y)P/In—Ga—P/GaPQDs. Following the principle of minimizing the lattice mismatch betweenthe core and the shell materials, ZnSe_(z)S_(1-z) alloy is used as theshell material, for which the lattice constant can be tuned according tothe Se/S ratio. The ZnSe_(z)S_(1-z) shell growth procedure involved theaddition of a (TOP-Se)_(z) and (TOP-S)_(1-z) mixture together withzinc-stearate to the crude reaction mixture of In_(x)Zn_(y)P/In—Ga—P/GaPQDs. The relative amount of Se and S (z) was chosen so that the latticeconstant of the shell would match or nearly match, as described above,the lattice constant of the In_(x)Zn_(y)P/In—Ga—P/GaP QDs.

FIG. 11A shows the absorption and emission spectra ofIn_(x)Zn_(y)P/In—Ga—P/GaP/ZnSe_(z)S_(1-z) core/multiple-shells QDs atdifferent shell reaction times. Upon the shell growth a marked increaseof the absorbance at wavelengths below 440 nm, corresponding to the bandgap of bulk ZnSe_(z)S_(1-z), was observed, proving the overgrowth of theexpected zinc sulphide selenide material. FIG. 11B shows the XRDpatterns observed for In_(x)Zn_(y)P QDs, In_(x)Zn_(y)P/In—Ga—P/GaP QDs,and In_(x)Zn_(y)P/In—Ga—P/GaP/ZnSe_(z)S_(1-z) QDs, which confirm notonly that the three samples have a zinc blende crystal structure, butalso that a lattice matched core/shell structures were formed, as noshift of XRD peaks was observed. TEM analysis further supported theformation of a ZnSe_(z)S_(1-z) shell as, after the shell growthprocedure nearly spherical QDs with a diameter of 4.6±0.6 nm wereobserved, indicating that a 0.6 nm shell has been grown. A thicker shell(1 nm), could also be grown via a multiple injection approach.

The resulting QDs were characterized by a PL emission peaked at 565 nmwith a full width at half maximum of 52 nm and a PL QY of up to 75%.Core/Shell QDs emitting at longer wavelength (620 nm) were alsosynthesized by using In_(x)Zn_(y)P cores emitting at λ>600 nm.

Reliability tests were performed on InP base core/shell without the GaPshell or the ZnSe_(z)S_(1-z) shell respectively. The results aresummarized in 11C. A dispersion of purified In_(x)Zn_(y)P/In—Ga—P/GaPQDs, In_(x)Zn_(y)P/ZnSe_(z)S_(1-z) QDs andIn_(x)Zn_(y)P/In—Ga—P/GaP/ZnSe_(z)S_(1-z) QDs in toluene were loaded,under ambient conditions, into a capillary, placed on the top of a GaNLED (lamp power 1 W/cm²; Temperature 50-60° C.) and the PL QY wasmonitored for 5 weeks. In case of In_(x)Zn_(y)P/In—Ga—P/GaP andIn_(x)Zn_(y)P/ZnSe_(z)S_(1-z) QDs the PL decreased after exposure.In_(x)Zn_(y)P/In—Ga—P/GaP/ZnSe_(z)S_(1-z) QDs showed prolonged stabilityas the PL QY, after an initial small drop of about 5% in the first hour,retained a constant PL QY of 70% for 5 weeks. The experiment illustratesmultishell QDs of In_(x)Zn_(y)P/In—Ga—P/GaP/ZnSe_(z)S_(1-z) may haveexcellent photostability.

Though the discussion herein refers to InP-based QDs, a promisingmaterial for lighting and display applications of QDs, the technique ofalloying QD cores to match the lattice of subsequent shells may beapplied to other material systems.

Any suitable shell material may be used in embodiments of the invention,including, for example, MgSe, ZnS, ZnSe, ZnTe, CdSe, CdS, GaP, GaN,GaAs, and GaSb.

Any suitable core material may be used in embodiments of the invention,including, for example, GaN, GaP, GaAs, GaSb, AlN, AlP, AlAs, AlSb, InN,InP, InAs, InSb, GaNP, GaNAs, GANSb, GaPAs, GaPSb, AlNP, AlNAs, ALNSb,AlPAs, AlPSb, InNP, InNAs, InNSb, InPAs, InPSb, GaAlNP, AlGaN, AlGaP,AlGaAs, AlGaSb, InGaN, InGaP, InGaAs, InGaSb, AlInN, AlInP, AlInAs,AlInSb, GaAlNAs, GaAlNSb, GaAlPAs, GaAlPSb, GaInNP, GaInNAs, GaInNSb,GaInPAs, GaInPSb, InAlNP, InAlNAs, InAlNSb, InAlPAs, InAlPSb, and othercombinations thereof.

The individual particles of the nanocrystal materials described hereinmay be any suitable shape including, for example, spheres, rods, sheets,triangles, etc. In some embodiments, the individual particles arespheres (quantum dots), which may luminesce more efficiently than othermaterial.

The nanocrystal materials described herein may be tuned to emitdifferent colors of light, for example by selecting the composition ofthe core material. In various embodiments, the nanocrystal materials maybe tuned to emit red, amber, green, or blue light.

The nanocrystal materials described herein emit light with a full widthhalf maximum (FWHM) of no more than 80 nm in some embodiments, no morethan 70 nm in some embodiments, no more than 65 nm in some embodiments,no more than 60 nm in some embodiments, and at least 10 nm in someembodiments.

The nanocrystal materials described herein may be used to formgiant-shell quantum dots, in some embodiments. In traditional core-shellstructures, the outer semiconductor shell may provide a higher band-gapinterface and may passivate the outer surface of the quantum dot core.When there is lattice mismatch between the core and the shell, the shellthickness is limited. For example, in a CdSe/ZnS quantum dot, increasingthe ZnS shell thickness beyond a nominal 3 monolayers (QD diameter 7˜10nm) often results in reduced quantum efficiency, because the latticemis-match between CdSe and ZnS prevents defect-free epitaxial growth ofthicker ZnS layers. The core QD diameter would typically be 3˜6 nm.

In giant shell QDs, the shell is much thicker. In a giant shell QD, theshell may be at least 5 monolayers thick in some embodiments, at least10 monolayers thick in some embodiments, at least 15 monolayers thick insome embodiments, at least 20 monolayers thick in some embodiments, andno more than 500 monolayers thick in some embodiments. The final QDdiameter may be 15˜20 nm in some embodiments, at least 10 nm in someembodiments, at least 15 nm in some embodiments, at least 20 nm in someembodiments, and no more than 50 nm in some embodiments.

Giant shell QDs generally have greater optical absorption within theshell relative to the core, as compared to traditional QDs, since theshell consists of larger percentage of the bulk mass in a giant shellQD.

Lattice matching between the core and shell may improve the quantumefficiency (brightness) and stability of a giant shell QD. For example,a lattice mismatched shell material energetically favors returning toits bulk crystal lattice, as opposed to following the template from thecore material. Hence, the lattice matching is perceived to be a keyingredient to allow for both large diameters and high QE.

The nanocrystal materials described herein may be used in asymmetric QDstructures (ie. Symmetric core+elongated rod-like shell). In suchstructures, during growth of the shell, a larger mass of shell materialis grown only on the portion of the QD core. This may allow for reducingthe overall stress on the layers as the lattice matching is not over theentire surface. FIG. 8(a) illustrates a core-shell QD, FIG. 8(b)illustrates a giant core-shell QD, and FIG. 8(c) illustrates anasymmetric core-shell QD.

In the discussion herein, the lattice mismatches may be calculated usinga core lattice constant determined from XRD measurements (having anuncertainty in the range 0.01-0.001 Å) and a shell lattice constanttaken from literature (Sadekar, H. K.; Ghule, A. V.; Sharma, R. J.Alloys Compd. 2011, 509 (18), 5525-5531) (for the given composition).The shell lattice constant in the nanosystems may differ from the bulkliterature values.

In some embodiments, the lattice mismatch may be reduced from less than1% to almost 0%. The lattice mismatch, defined as[(a_(core)−a_(shell))/a_(shell)]*100%, may be no more than 1.7% in someembodiments, no more than 1.5% in some embodiments, no more than 1% insome embodiments, no more than 0.7% in some embodiments, no more than0.5% in some embodiments, and 0% in some embodiments (lattice match). Inthe above equation, a_(core) refers to the actual lattice constant inthe as-grown core, and a_(shell) refers to the actual lattice constantin the as-grown shell. Lattice engineering of the core allows for strainfree epitaxial growth of functional shell materials, including ZnSe, GaPand ZnS. In some embodiments, photoluminescence quantum yields may bemaximal, up to 60%, when the lattice constant of In_(x)Zn_(y)P coresmatches that of a ZnSe_(z)S_(1-z) shell.

Some benefits of embodiments of the invention may include (1) defectfree core-shell structures over alloyed InZnP QD cores; (2) large“giant” QDs afforded by defect free shell layer over core of alloyedInZnP QD cores; (3) asymmetric QD structures (rod, tetrapod, wire, etc)using alloyed InZnP QD cores; (4) improved QE and stability from QDstructures using alloyed InZnP QD cores; and (5) a simple one-pot methodfor the synthesis of zinc-blende In_(x)Zn_(y)P alloyed nanocrystals withtunable lattice parameters. Other benefits are contemplated and withinthe scope of the invention.

Though the examples and embodiments herein refer to replacing an atom inthe lattice with an atom with a smaller ionic radius, in someembodiments, the lattice constant may be changed by replacing an atomwith a larger ionic radius.

The luminescent materials described herein may absorb light of a firstwavelength and emit light of a different, second wavelength, which maybe a different color from the first wavelength. The luminescentmaterials may be combined with a light source such as a light emittingdiode (LED), according to some embodiments.

FIG. 4 illustrates a III-nitride LED 1 that may be used with theabove-described luminescent materials in embodiments of the presentinvention. Any suitable semiconductor light emitting device may be usedand embodiments of the invention are not limited to the deviceillustrated in FIG. 4. The device of FIG. 4 is formed by growing aIII-nitride semiconductor structure on a growth substrate 10 as is knownin the art. The growth substrate is often sapphire but may be anysuitable substrate such as, for example, SiC, Si, GaN, or a compositesubstrate. A surface of the growth substrate on which the III-nitridesemiconductor structure is grown may be patterned, roughened, ortextured before growth, which may improve light extraction from thedevice. A surface of the growth substrate opposite the growth surface(i.e. the surface through which a majority of light is extracted in aflip chip configuration) may be patterned, roughened or textured beforeor after growth, which may improve light extraction from the device.

The semiconductor structure includes a light emitting or active regionsandwiched between n- and p-type regions. An n-type region 16 may begrown first and may include multiple layers of different compositionsand dopant concentration including, for example, preparation layers suchas buffer layers or nucleation layers, and/or layers designed tofacilitate removal of the growth substrate, which may be n-type or notintentionally doped, and n- or even p-type device layers designed forparticular optical, material, or electrical properties desirable for thelight emitting region to efficiently emit light. A light emitting oractive region 18 is grown over the n-type region. Examples of suitablelight emitting regions include a single thick or thin light emittinglayer, or a multiple quantum well light emitting region includingmultiple thin or thick light emitting layers separated by barrierlayers. A p-type region 20 may then be grown over the light emittingregion. Like the n-type region, the p-type region may include multiplelayers of different composition, thickness, and dopant concentration,including layers that are not intentionally doped, or n-type layers.

After growth, a p-contact is formed on the surface of the p-type region.The p-contact 21 often includes multiple conductive layers such as areflective metal and a guard metal which may prevent or reduceelectromigration of the reflective metal. The reflective metal is oftensilver but any suitable material or materials may be used. After formingthe p-contact 21, a portion of the p-contact 21, the p-type region 20,and the active region 18 is removed to expose a portion of the n-typeregion 16 on which an n-contact 22 is formed. The n- and p-contacts 22and 21 are electrically isolated from each other by a gap 25 which maybe filled with a dielectric such as an oxide of silicon or any othersuitable material. Multiple n-contact vias may be formed; the n- andp-contacts 22 and 21 are not limited to the arrangement illustrated inFIG. 4. The n- and p-contacts may be redistributed to form bond padswith a dielectric/metal stack, as is known in the art.

In order to form electrical connections to the LED 1, one or moreinterconnects 26 and 28 are formed on or electrically connected to then- and p-contacts 22 and 21. Interconnect 26 is electrically connectedto n-contact 22. Interconnect 28 is electrically connected to p-contact21. Interconnects 26 and 28 are electrically isolated from the n- andp-contacts 22 and 21 and from each other by dielectric layer 24 and gap27. Interconnects 26 and 28 may be, for example, solder, stud bumps,gold layers, or any other suitable structure.

The substrate 10 may be thinned or entirely removed. In someembodiments, the surface of substrate 10 exposed by thinning ispatterned, textured, or roughened to improve light extraction.

Any suitable light emitting device may be used in light sourcesaccording to embodiments of the invention. The invention is not limitedto the particular LED illustrated in FIG. 4. The light source, such as,for example, the LED illustrated in FIG. 4, is illustrated in thefollowing figures by block 1.

FIGS. 5, 6, and 7 illustrate devices that combine an LED 1 and awavelength converting structure 30. The wavelength converting structure30 may include a luminescent material such as nanocrystal luminescentmaterials according to the embodiments and examples described herein.

The wavelength converting structure may be, for example, one or moreluminescent materials disposed in transparent material such as siliconeor glass that is rolled, cast, or otherwise formed into a sheet, thensingulated into individual wavelength converting structures; one or moreluminescent materials that are disposed in a transparent material suchas silicone that is formed into a flexible sheet, which may be laminatedor otherwise disposed in the path of light from an LED 1, one or moreluminescent materials that are mixed with a transparent material such assilicone and dispensed, screen printed, stenciled, molded, or otherwisedisposed over LED 1, or on a transparent plate that may be disposed inthe path of light from an LED 1; and luminescent materials that arecoated on LED 1 or another structure by electrophoretic, vapor, or anyother suitable type of deposition.

In FIG. 5, the wavelength converting structure 30 is directly connectedto the LED 1. For example, the wavelength converting structure may bedirectly connected to the substrate 10 illustrated in FIG. 4, or to thesemiconductor structure, if the substrate 10 is removed.

In FIG. 6, the wavelength converting structure 30 is disposed in closeproximity to LED 1, but not directly connected to the LED 1. Forexample, the wavelength converting structure 30 may be separated fromLED 1 by an adhesive layer 32, a small air gap, a transparent plate thatsupports the wavelength converting structure 30, or any other suitablestructure. The spacing between LED 1 and the wavelength convertingstructure 30 may be, for example, less than 500 μm in some embodiments.

In FIG. 7, the wavelength converting structure 30 is spaced apart fromLED 1. The spacing between LED 1 and the wavelength converting structure30 may be, for example, on the order of millimeters in some embodiments.Such a device may be referred to as a “remote phosphor” device. Remotephosphor arrangements may be used, for example, in backlights fordisplays.

The wavelength converting structure 30 may be square, rectangular,polygonal, hexagonal, circular, or any other suitable shape. Thewavelength converting structure may be the same size as LED 1, largerthan LED 1, or smaller than LED 1.

Multiple wavelength converting materials and multiple wavelengthconverting structures can be used in a single device. For example,multiple wavelength converting structures as described above may be usedin a single device, and/or the wavelength converting structuresdescribed above may be combined with other wavelength convertingstructures such as, for example, luminescent ceramics, powder phosphors,or any other suitable structure.

In addition to luminescent materials described herein, a device may alsoinclude other wavelength converting materials such as, for example,conventional phosphors, organic phosphors, dyes, organic semiconductors,II-VI or III-V semiconductors, Si, II-VI, or III-V semiconductor quantumdots or nanocrystals, polymers, or other materials that luminesce.

The wavelength converting materials absorb light emitted by the LED andemit light of one or more different wavelengths. Unconverted lightemitted by the LED is often part of the final spectrum of lightextracted from the structure, though it need not be. Examples of commoncombinations include a blue-emitting LED combined with a yellow-emittingwavelength converting material, a blue-emitting LED combined with green-and red-emitting wavelength converting materials, a UV-emitting LEDcombined with blue- and yellow-emitting wavelength converting materials,and a UV-emitting LED combined with blue-, green-, and red-emittingwavelength converting materials. Wavelength converting materialsemitting other colors of light may be added to tailor the spectrum oflight extracted from the structure.

Multiple wavelength converting materials may be mixed together or formedas separate structures.

In some embodiments, other materials may be added to the wavelengthconverting structure or the device, such as, for example, materials thatimprove optical performance, materials that encourage scattering, and/ormaterials that improve thermal performance.

EXAMPLES

In an example of typical synthesis, tris(trimethylsilyl)phosphine(P(TMS)₃) was injected into a solution of indium acetate (In(OAc)₃),zinc acetate (Zn(OAc)₂) and palmitic acid (In:Zn:PA=1:0.5:3) at 300° C.Indium acetate (0.12 mmol), zinc acetate (0.06 mmol) and palmitic acid(0.36 mmol) were mixed in octadecene (ODE), and kept under vacuum for 2h at 130° C. In a N₂ purged glove box a solution of P(TMS)₃ (In:P=2:1)in 1 mL of ODE was prepared and loaded into a syringe. After degassing,the temperature was raised to 300° C. The phosphorus precursor was thenrapidly injected into the reaction mixture and the temperature wasreduced and maintained at 270° C. for 2 h. While keeping the amount ofindium fixed, the Zn/In precursor ratio was varied between 0 and 5, orbetween 0 and 10. The resulting In_(x)Zn_(y)P NCs were washed threetimes by addition of ethanol and acetone to induce precipitation,followed by dispersion in toluene. As an additional washing step theorganic ligands were stripped and replaced with S²⁻ ions through theaddition of (NH₄)₂S, which allows the removal of unreacted species.

Preparation of In_(x)Zn_(y)P QDs, with different Zn/In ratios (0, 0.5,3) in the range of 0<Zn/In<10.

Example 1, InP core synthesis (y/x=0). In a three-neck flask 35 mgIn(OAc)₃ (0.12 mmol), and 91 mg palmitic acid (0.36 mmol) were mixed in8 mL 1-octadecene. The solution was degassed under vacuum for an hour at100° C. After heating up the solution to 300° C. under nitrogen flow, 17μL (P(TMS)₃) (0.06 mmol; 15 mg) in 1 mL ODE was rapidly injected. Thetemperature was then lowered to 270° C. and held for 2 h. The InP NCswere washed three times by dispersion in toluene followed byprecipitation by addition of a mixture ethanol:acetone (1:3), and storedin toluene or hexane in a N₂ filled vial in the glovebox. The obtainednanocrystal (QD) has a UV first absorption maximum around 540 nm, andlattice constant of 5.928 Å.

Example 2, In_(x)Zn_(y)P core synthesis (y/x=0.5). In a three-neck flask35 mg In(OAc)₃ (0.12 mmol), 11 mg Zn(OAc)₂ (0.06 mmol) and 91 mgpalmitic acid (0.36 mmol) were mixed in 8 mL 1-octadecene. The solutionwas degassed under vacuum for an hour at 100° C. After heating up thesolution to 300° C. under nitrogen flow, 17 μL (P(TMS)₃) (0.06 mmol; 15mg) in 1 mL ODE was rapidly injected. The temperature was then loweredto 270° C. and held for 2 h. The In_(x)Zn_(y)P NCs were washed threetimes by dispersion in toluene followed by precipitation by addition ofa mixture ethanol:acetone (1:3), and stored in toluene or hexane in a N₂filled vial in the glovebox. The obtained nanocrystal (QD) has a UVfirst absorption maximum around 503 nm, and a lattice constant of 5.863Å.

Example 3, In_(x)Zn_(y)P core synthesis (y/x=2.8). In a three-neck flask35 mg In(OAc)₃ (0.12 mmol), 66 mg Zn(OAc)₂ (0.36 mmol) and 91 mgpalmitic acid (0.36 mmol) were mixed in 8 mL 1-octadecene. The solutionwas degassed under vacuum for an hour at 100° C. After heating up thesolution to 300° C. under nitrogen flow, 17 μL (P(TMS)₃) (0.06 mmol; 15mg) in 1 mL ODE was rapidly injected. The temperature was then loweredto 270° C. and held for 2 h. The In_(x)Zn_(y)P NCs were washed threetimes by dispersion in toluene followed by precipitation by addition ofa mixture ethanol:acetone (1:3), and stored in toluene or hexane in a N₂filled vial in the glovebox. The obtained nanocrystal (QD) has a UVfirst absorption maximum around 517 nm, and a lattice constant of 5.497Å.

The amount of zinc precursors was varied between 0 mg (for Zn/In=0) and220 mg (for Zn/In=10), while the In(OAc)₃ and P(TMS)₃ were keptconstant.

In the examples below, different cores were used for the fabrication ofa core shell structure. The cores match shells with differentcomposition: ZnSe_(0.51)S_(0.49) shells in case of In_(x)Zn_(y)P QDcores (y/x=2.8), ZnSe_(0.2)S_(0.8) shells in case of In_(x)Zn_(y)P QDcores (y/x=3.6), and ZnSe_(0.8)S_(0.2) shells in case of In_(x)Zn_(y)PQD cores (y/x=2). The shell composition was varied to demonstrate thatthe highest values of QY was obtained when the core and the shell match.

Preparation of In_(x)Zn_(y)P QDs (y/x=2.8) core with ZnSe_(z)S_(z-1)shell.

Example 4, preparation of In_(x)Zn_(y)P QDs (y/x=2.8) core with latticeconstant 5.497 Å and a ZnS shell with lattice constant a: 5.407 Å. For asynthesis with z=0, 0.325 g of Zn stearate in 1.5 mL of ODE was addedinto a three neck flask containing 2 ml of as synthesized In_(x)Zn_(y)Pcore at room temperature. The temperature was then set to 300° C. with arate of 10° C./min. When the temperature was about 90° C., 0.5 mL of 4Msolution of TOP-S was injected into the reaction mixture. The reactionwas kept at 300° C. for 20 min, and subsequently quenched by loweringthe temperature. The product was purified by dispersion in chloroform (2mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 518 nm and QY: 41.4%.

Example 5, preparation of In_(x)Zn_(y)P QDs (y/x=2.8) core with latticeconstant 5.497 Å and a ZnSe_(0.6)S_(0.4) shell with lattice constant a:5.535 Å. For a synthesis with z=0.6, 0.325 g of Zn stearate in 1.5 mL ofODE was added into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.3 mL of 4M solution of TOP-Se and 0.2 mL of a 4 ML solution ofTOP-S were simultaneously injected into the reaction mixture. Thereaction was kept at 300° C. for 20 min, and subsequently quenched bylowering the temperature. The product was purified by dispersion inchloroform (2 mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 547 nm and QY: 49.2%.

Example 6, preparation of In_(x)Zn_(y)P QDs (y/x=2.8) core with latticeconstant 5.497 Å and a ZnSe_(0.4)S_(0.6) shell with lattice constant a:5.464 Å. For a synthesis with z=0.4, 0.325 g of Zn stearate in 1.5 mL ofODE was added into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.20 mL of 4M solution of TOP-Se and 0.30 mL of a 4 ML solution ofTOP-S were simultaneously injected into the reaction mixture. Thereaction was kept at 300° C. for 20 min, and subsequently quenched bylowering the temperature. The product was purified by dispersion inchloroform (2 mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 551 nm and QY: 59.2%.

Example 7, preparation of In_(x)Zn_(y)P QDs (y/x=2.8) core with latticeconstant 5.497 Å and a ZnSe_(0.51)S_(0.49) shell with lattice constanta: 5.4971 Å. For a synthesis with z=0.6, 0.325 g of Zn stearate in 1.5mL of ODE was added into a three neck flask containing 2 ml of assynthesized In_(x)Zn_(y)P core at room temperature. The temperature wasthen set to 300° C. with a rate of 10° C./min. When the temperature wasabout 90° C., 0.255 mL of 4M solution of TOP-Se and 0.245 mL of a 4 MLsolution of TOP-S were simultaneously injected into the reactionmixture. The reaction was kept at 300° C. for 20 min, and subsequentlyquenched by lowering the temperature. The product was purified bydispersion in chloroform (2 mL) followed by precipitation by addition ofa mixture of ethanol:acetone (1:4). The obtained nanocrystal (QD) has amaximum PL emission at 552 nm and QY: 60%.

Preparation of In_(x)Zn_(y)P QDs (y/x=3.6) core with ZnSe_(z)S_(1-z)shell.

Example 8, preparation of In_(x)Zn_(y)P QDs (y/x=3.6) core with latticeconstant 5.449 Å and a ZnS shell with lattice constant a: 5.407 Å. For asynthesis with z=0, 0.325 g of Zn stearate in 1.5 mL of ODE was addedinto a three neck flask containing 2 ml of as synthesized In_(x)Zn_(y)Pcore at room temperature. The temperature was then set to 300° C. with arate of 10° C./min. When the temperature was about 90° C., 0.5 mL of 4Msolution of TOP-S was injected into the reaction mixture. The reactionwas kept at 300° C. for 20 min, and subsequently quenched by loweringthe temperature. The product was purified by dispersion in chloroform (2mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 518 nm and QY: 25.4%.

Example 9, preparation of In_(x)Zn_(y)P QDs (y/x=3.6) core with latticeconstant 5.449 Å and a ZnSe_(0.2)S_(0.8) shell with lattice constant a:5.435 Å. For a synthesis with z=0.2, 0.325 g of Zn stearate in 1.5 mL ofODE was added into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.10 mL of 4M solution of TOP-Se and 0.40 mL of a 4 ML solution ofTOP-S were simultaneously injected into the reaction mixture. Thereaction was kept at 300° C. for 20 min, and subsequently quenched bylowering the temperature. The product was purified by dispersion inchloroform (2 mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 547 nm and QY: 45.2%.

Example 10, preparation of In_(x)Zn_(y)P QDs (y/x=3.6) core with latticeconstant 5.449 Å and a ZnSe_(0.4)S_(0.6) shell with lattice constant a:5.464 Å. For a synthesis with z=0.4, 0.325 g of Zn stearate in 1.5 mL ofODE was added into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.20 mL of 4M solution of TOP-Se and 0.30 mL of a 4 ML solution ofTOP-S were simultaneously injected into the reaction mixture. Thereaction was kept at 300° C. for 20 min, and subsequently quenched bylowering the temperature. The product was purified by dispersion inchloroform (2 mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 551 nm and QY: 36.2%.

Example 11, preparation of In_(x)Zn_(y)P QDs (y/x=3.6) core with latticeconstant 5.449 Å and a ZnSe_(0.8)S_(0.2) shell with lattice constant a:5.572 Å. For a synthesis with z=0.6, 0.325 g of Zn stearate in 1.5 mL ofODE was added into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.40 mL of 4M solution of TOP-Se and 0.10 mL of a 4 ML solution ofTOP-S were simultaneously injected into the reaction mixture. Thereaction was kept at 300° C. for 20 min, and subsequently quenched bylowering the temperature. The product was purified by dispersion inchloroform (2 mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 552 nm and QY: 19%.

Example 12, preparation of In_(x)Zn_(y)P QDs (y/x=3.6) core with latticeconstant 5.449 Å and a ZnSe shell with lattice constant a: 5.670 Å. Fora synthesis with z=0.6, 0.325 g of Zn stearate in 1.5 mL of ODE wasadded into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.5 mL of 4M solution of TOP-Se was injected into the reactionmixture. The reaction was kept at 300° C. for 20 min, and subsequentlyquenched by lowering the temperature. The product was purified bydispersion in chloroform (2 mL) followed by precipitation by addition ofa mixture of ethanol:acetone (1:4). The obtained nanocrystal (QD) has amaximum PL emission at 552 nm and QY: 18%.

Preparation of In_(x)Zn_(y)P QDs (y/x=2) core with ZnSe_(z)S_(1-z)shell.

Example 13, preparation of In_(x)Zn_(y)P QDs (y/x=2) core with latticeconstant 5.601 Å and a ZnS shell with lattice constant a: 5.407 Å. For asynthesis with z=0, 0.325 g of Zn stearate in 1.5 mL of ODE was addedinto a three next flask containing 2 ml of as synthesized In_(x)Zn_(y)Pcore at room temperature. The temperature was then set to 300° C. with arate of 10° C./min. When the temperature was about 90° C., 0.5 mL of 4Msolution of TOP-S was injected into the reaction mixture. The reactionwas kept at 300° C. for 20 min, and subsequently quenched by loweringthe temperature. The product was purified by dispersion in chloroform (2mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 518 nm and QY: 20.5%.

Example 14, preparation of In_(x)Zn_(y)P QDs (y/x=2) core with latticeconstant 5.601 Å and a ZnSe_(0.4)S_(0.6) shell with lattice constant a:5.464 Å. For a synthesis with z=0.6, 0.325 g of Zn stearate in 1.5 mL ofODE was added into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.2 mL of 4M solution of TOP-Se and 0.3 mL of a 4 ML solution ofTOP-S were simultaneously injected into the reaction mixture. Thereaction was kept at 300° C. for 20 min, and subsequently quenched bylowering the temperature. The product was purified by dispersion inchloroform (2 mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 552 nm and QY: 26.4%.

Example 15, preparation of In_(x)Zn_(y)P QDs (y/x=2) core with latticeconstant 5.601 Å and a ZnSe_(0.8)S_(0.2) shell with lattice constant a:5.572 Å. For a synthesis with z=0.6, 0.325 g of Zn stearate in 1.5 mL ofODE was added into a three neck flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P core at room temperature. The temperature was then set to300° C. with a rate of 10° C./min. When the temperature was about 90°C., 0.4 mL of 4M solution of TOP-Se and 0.1 mL of a 4 ML solution ofTOP-S were simultaneously injected into the reaction mixture. Thereaction was kept at 300° C. for 20 min, and subsequently quenched bylowering the temperature. The product was purified by dispersion inchloroform (2 mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 552 nm and QY: 41%.

Example 16, preparation of In_(x)Zn_(y)P QDs (y/x=2) core with latticeconstant 5.601 Å and a ZnSe shell with lattice constant a: 5.670 Å. Fora synthesis with z=0, 0.325 g of Zn stearate in 1.5 mL of ODE was addedinto a three next flask containing 2 ml of as synthesized In_(x)Zn_(y)Pcore at room temperature. The temperature was then set to 300° C. with arate of 10° C./min. When the temperature was about 90° C., 0.5 mL of 4 Msolution of TOP-Se was injected into the reaction mixture. The reactionwas kept at 300° C. for 20 min, and subsequently quenched by loweringthe temperature. The product was purified by dispersion in chloroform (2mL) followed by precipitation by addition of a mixture ofethanol:acetone (1:4). The obtained nanocrystal (QD) has a maximum PLemission at 518 nm and QY: 34%.

Preparation of In_(x)Zn_(y)P QDs (y/x=2.8) core with ZnSe_(z)S_(z-1)Giant-shell.

Example 17, preparation of In_(x)Zn_(y)P QDs (y/x=2.8) core with latticeconstant 5.497 Å and a ZnSe_(0.51)S_(0.49) giant shell with latticeconstant a: 5.4971 Å. For a synthesis with z=0.6, 0.325 g of Zn stearatein 1.5 mL of ODE was added into a three neck flask containing 2 ml of assynthesized In_(x)Zn_(y)P core at room temperature. The temperature wasthen set to 300° C. with a rate of 10° C./min. When the temperature wasabout 90° C., 0.255 mL of 4M solution of TOP-Se and 0.245 mL of a 4 MLsolution of TOP-S were simultaneously injected into the reactionmixture. The shell was annealed at 300° C. for 20 min. The temperaturewas then lowered at 100° C. and the same procedure was repeated for theadditional shells layers. The amount of Zn precursor for the shelladdition cycles 2 and 3 were as follows: 0.75 g and 1.5 g in 5 mL ofODE, respectively. In case of the Se and S precursor, the amounts were0.50 mL (TOP-Se) and 0.49 mL (TOP-S) for the second cycle, and 1.02 mL(TOP-Se) and 0.98 mL (TOP-S) for the third cycle. The product waspurified by dispersion in chloroform (5 mL) followed by precipitation byaddition of a mixture of ethanol:acetone (1:4).

Example 18, red emitting In_(x)Zn_(y)P core synthesis (y/x=1).Red-emitting, giant shell QDs are formed as follows: for growth of thesynthesized InP cores a stock solution may be made containing 292 mg (1mmol) of In(OAc)₃, 184 mg (1 mmol) of Zn(OAc)₂ and 769 mg (3 mmol) of PAin 10 mL of ODE in a three-neck round-bottom flask. The mixture may beput under vacuum for 2 hours at 130° C. After two hours the mixture maybe put under dried nitrogen gas and heated to 250° C. to dissolve thesalts and to form the palmitate complex. After dissolution, the solutionmay be cooled. The P(TMS)₃ precursor may be made by diluting (145 μL(0.5 mmol) P(TMS)₃P in 10 mL of ODE in the glovebox. After the synthesisof the In_(x)Zn_(y)P cores, the temperature of the core solution may belowered to 250° C. 1 mL of the In—Zn palmitate stock solution may beinjected dropwise into the core solution in 6 minutes. After 10 minutes,1 mL of the P(TMS)₃ precursor solution may be injected dropwise in theIn_(x)Zn_(y)P core solution over a time span of 40 minutes. The sameprocedure may be followed several time until the particles reached thedesirable size. The obtained nanocrystal (QD) may have a UV firstabsorption maximum around 540 nm, and lattice constant of 5.576 Å.

Example 19, Synthesis with intermediate Ga-containing layer. InxZnyP QDswere synthesized by any suitable method, such as: 35 mg of In(OAc)3(0.12 mmol), a desired amount of Zn(OAc)₂ and 91 mg of palmitic acid(0.36 mmol) were mixed together with 8 mL of 1-octadecene in athree-neck flask. The solution was degassed under vacuum for 1 hour at100° C. After heating up the reaction mixture to 300° C. under nitrogenflow, 17 μL of (P(TMS)₃) (0.06 mmol; 15 mg) in 1 mL of ODE were rapidlyinjected into the flask. The temperature was then lowered to 270° C. andthe NCs were allowed to grow for 2 h. This “hot” crude reaction solutionwas immediately used for the cation exchange reactions or for thesynthesis of red emitting QDs. Alternatively, to collect theIn_(x)Zn_(y)P QDs, the reaction flask was rapidly cooled to roomtemperature and the NCs were washed three times by dispersion in toluenefollowed by precipitation by addition of a mixture ethanol:acetone(1:3), and eventually stored in toluene (or hexane) in a N₂ filledglovebox. The amount of zinc precursor was varied from 0 mg (forZn/In=0) to 36 mg (for Zn/In=1.5), while the amounts of In(OAc)₃ andP(TMS)₃ were kept constant.

Preparation of the In—Zn palmitate (In:Zn=1:1) and P(TMS)₃ precursors: AIn—Zn palmitate stock solution was prepared by mixing 292 mg (1 mmol) ofIn(OAc)₃, 184 mg (1 mmol) of Zn(OAc)₂ and 769 mg (3 mmol) of PA in 10 mLof ODE in a three-neck round-bottom flask. The mixture was degassedunder vacuum at 130° C. for two hours and then heated to 250° C. underN₂ in order to form the In—Zn palmitate complexs. After completedissolution of metal precursors, the solution was cooled to roomtemperature and stored in a N₂ filled glove box. A P(TMS)₃ precursorsolution was prepared by diluting 145 μL (0.5 mmol) of P(TMS)3P in 10 mLof ODE.

Growth of In_(x)Zn_(y)P cores: In order to further increase the size ofas-synthesized In_(x)Zn_(y)P QDs, a multiple injection route wasadopted. The temperature of the crude “hot” reaction mixture was loweredto 250° C. and 1 mL of the In—Zn palmitate stock solution was injecteddropwise into the flask in 6 minutes. After 10 minutes, 1 mL of theP(TMS)₃ precursor solution was injected dropwise in the reaction flaskover a time span of 40 minutes. The same procedure was followed severaltime till the particles reached the desirable size.

Cation exchange reaction between Zn²⁺ and Ga³⁺: A 0.2 M galliumprecursor solution was prepared by dissolving GaCl₃ (3 mmol, 528 mg) inoleic acid (12 mmol, 3.39 g) and 20 mL ODE at 140° C. for 1 h. Thetemperature of the crude “hot” reaction mixture was lowered to 200° C.and 230 μL of Gallium precursor solution (containing 0.03 mmol of Ga³⁺)were added dropwise. The reaction was kept for 1 hour after which other230 μL of Gallium precursor solution (containing 0.03 mmol of Ga³⁺) wereadded. Subsequent injections of Ga precursor solution were performedfollowing the same procedure for a total of 0.15 mmol of Ga(OA)₃ added.

Synthesis of In_(x)Zn_(y)P/GaP core/shell QDs: The temperature of thecrude “hot” reaction mixture was lowered to 200° C. and 230 μL ofGallium precursor solution (containing 0.03 mmol of Ga³⁺) were addeddropwise. The temperature was kept at 200° C. for 1 h. This was repeated3 times for a total amount of 0.09 mmol of gallium added. Subsequently,0.03 mmol of P(TMS)₃ diluted in 1 mL of ODE were added at 150° C. andreacted at 200° C. Subsequent injection of Ga and P precursor wereperformed following the same procedure.

Synthesis of In_(x)Zn_(y)P/GaP/ZnSe_(z)S_(1-z) core/shell/shell QDs: Theselenium and sulphur precursor solutions, used for the ZnSe_(z)S_(1-z)shell growth, were prepared as follow: in a reaction flask a 1M TOP-Se(or S) was prepared by dissolving 4 mmol of Se (or S) powder in 4 mL ofTOP. In a typical synthesis, 0.325 g of Zn stearate in 1.5 mL of ODE,were added into a three next flask containing 2 ml of as synthesizedIn_(x)Zn_(y)P/GaP QDs at room temperature. At this point the temperatureof the crude “hot” reaction mixture was set to 300° C. with a heatingrate of 10° C./min. When the temperature reached 90° C., a total of 0.5mL of the anions stock solution (Se-TOP+S-TOP) were added. TheZnSe_(z)S_(1-z) shell composition was changed by varying the Se-TOP andS-TOP precursors amounts: for example in case of z=0, 0.5 mL of 1M TOP-Swas added, while in case of z=0.5, 0.25 mL of 1M TOP-Se and 0.25 mL of1M TOP-S were added. The reaction was kept at 300° C. for 20 min, andsubsequently quenched by cooling the flask to room temperature. Theresulting QDs were purified by dispersion in chloroform (2 mL) followedby precipitation by addition of a mixture of ethanol:acetone (1:4). Theobtained QDs were stored in toluene in a N₂ filled vial in the glovebox.

Ligand exchange: A colloidal dispersion of washed NCs with organicligands was prepared in nonpolar solvents like toluene, while thesolution of inorganic ligands was prepared in polar formamide (FA)immiscible with toluene. The exchange of original organic ligands withS²⁻ inorganic species was carried out in a N₂ glove box. 20 μl of(NH₄)₂S solution was added to 1 mL of formamide (FA) and mixed with 1 mlof a QDs dispersion in toluene. The biphasic mixture was sonicated for15 minutes in a sonic bath at 60° C., leading to a complete phasetransfer of the NCs from toluene to the FA phase. The phase transfer canbe easily monitored by the color change of toluene (red to colorless)and FA (colorless to red) phases. The FA phase was separated and acetonewas added as non-solvent to precipitate the particles. To remove theresidual organic ligands a further washing step with toluene wasapplied. This was repeated twice. Finally, the QDs were precipitated alast time by adding acetone as a non-solvent and re-dispersed indimethylformamide (DMF) for further analysis and stored in a N₂ filledvial in the glovebox.

The numerical values in the examples described herein may form the endpoints of ranges for the given value, in some embodiments.

FIG. 9(a) illustrates normalized absorption and normalized PL spectra ofIn_(x)Zn_(y)P QDs with different Zn²⁺ concentration. FIG. 9(b) is a plotof the λ,max (nm) for the absorption and PL emission wavelengths asfunction of the Zn/In molar ratio obtained by ICP(OES) analysis. FIG.9(c) is a plot of the PL QY (%) of In_(x)Zn_(y)P QDs as function of theZn/In molar ratio obtained by ICP(OES) analysis.

FIG. 10 is a plot of absorption (left) and PL emission (right) ofIn_(x)Zn_(y)P core with Zn/In:2.8 and In_(x)Zn_(y)P/ZnSe_(0.51)S_(0.49)core-shell.

Having described the invention in detail, those skilled in the art willappreciate that, given the present disclosure, modifications may be madeto the invention without departing from the spirit of the inventiveconcept described herein. Therefore, it is not intended that the scopeof the invention be limited to the specific embodiments illustrated anddescribed.

The invention claimed is:
 1. A luminescent structure comprising: anIn_(x)Zn_(y)P core, wherein 0≤y/x<100, and wherein the In_(x)Zn_(y)Pcore comprises an alloy including both In and Zn; and a shell disposedon a surface of the core, wherein a difference between a latticeconstant of the shell and a lattice constant of the In_(x)Zn_(y)P coreis less than 1.7% relative to the lattice constant of the shell.
 2. Theluminescent structure of claim 1 wherein 2≤y/x≤10.
 3. The luminescentstructure of claim 1 further comprising an intermediate layer disposedbetween the shell and the In_(x)Zn_(y)P core, wherein the intermediatelayer comprises Ga.
 4. The luminescent structure of claim 1 wherein theshell is lattice-matched to the In_(x)Zn_(y)P core.
 5. The luminescentstructure of claim 1 wherein the shell comprises ZnSe_(z)S_(1-z) whereinz=0-1.
 6. The luminescent structure of claim 5 wherein the shell furthercomprises GaP.
 7. The luminescent structure of claim 1 wherein the shellcomprises GaP.
 8. The luminescent structure of claim 1 wherein InP andZnP form an alloy.
 9. The luminescent structure of claim 1 wherein theIn_(x)Zn_(y)P core comprises Zn²⁺ incorporated into the crystal latticeof an InP quantum dot.
 10. The luminescent structure of claim 1 whereinthe In_(x)Zn_(y)P core is zinc blende.
 11. The luminescent structure ofclaim 1 wherein y and x are not both equal to
 1. 12. The luminescentstructure of claim 1 wherein the In_(x)Zn_(y)P core consists of an alloyconsisting of In, Zn, and P.
 13. A structure comprising: a semiconductorlight emitting device; and a nanocrystal disposed in a path of lightemitted by the light emitting device, the nanocrystal comprising: anInZnP core consisting of an InZnP alloy; and a shell disposed on asurface of the core, wherein a difference between a lattice constant ofthe shell and a lattice constant of the core is less than 1.7% relativeto the lattice constant of the shell.
 14. A method of forming aluminescent quantum dot material, the method comprising: providing anIn_(x)Zn_(x)P core, wherein 0≤y/x≤10, and wherein the In_(x)Zn_(y)P corecomprises an alloy including both In and Zn, surrounding theIn_(x)Zn_(y)P core with a shell, wherein a difference between a latticeconstant of the shell and a lattice constant of the In_(x)Zn_(y)P coreis less than 1.7% relative to the lattice constant of the shell.
 15. Themethod of claim 14 further comprising determining a lattice constant ofthe shell material composition.
 16. The method of claim 14 wherein thecore material comprises a group 12 material, a group 13 material, and agroup 15 material.
 17. The method of claim 16 wherein the group 12material, the group 13 material, and the group 15 material form analloy, such that the composition in the core material is substantiallyuniform through the core material.
 18. The method of claim 14 furthercomprising tuning the lattice constant of the core by adjusting theconcentration of precursor ratio of In/Zn during synthesis of the core.